用共振增强多光子电离方法研究几种含溴化合物的光解

利用飞行时间质谱仪(TOF)和共振增强多光子电离(REMPI)方法, 研究了两种正一溴代烷烃(C₂H₅Br, n-C₃H₇Br)和溴苯(C₆H₅Br)在234及267 nm附近的光解. 测出了这几种含溴化合物在不同波长下光解产物Br^*和Br的分支比N(Br*)/N(Br), 并根据从头计算结果, 解释了这几种含溴化合物光解产物的分支比随光解波长变化的趋势及几个低激发态势能面之间的关系.     

正-溴代烷烃的紫外光解动力学研究

利用共振增强多光子电离飞行时间质谱(REMPI-TOFMS)，研究了长链正-溴代烷烃R-Br(R为正烷烃基)(C2H5Br，n-C3H7Br，n-C4H9Br)在234及267nm附近的光解动力学．溴碎片来源于R-Br的直接解离：R-Br→R Br(^2P3/2)／Br(^2P1/2)，根据测定的离子信号强度，得到了Br^n与Br的分支比N(Br^*)／N(Br)及相应的相对量子产额φ(Br^*)和φ(Br)．φ(Br^*)与激光波长及分子结构显示了一定的依赖关系，将实验结果用CH3Br的解离模型进行拟合，得到了长链R-Br的光解动力学行为的定性解释。     

离子速度成像方法研究溴代环己烷的紫外光解动力学

利用二维离子速度成像方法对C6H11Br分子在234 nm附近的光解动力学行为进行了研究. 通过(2+1)共振增强多光子电离探测了光解产物Br*(2P1/2)和Br(2P3/2), 得到它们的相对量子产率. 从光解产物Br*(2P1/2)和Br(2P3/2)的速度图像得到了能量和角度分布. 结果表明, Br*原子主要来自于S1态的直接解离, 而Br则绝大部分是从S2态向T3态的系间交叉跃迁得到, 并导致了两种解离通道能量分布的差别. 实验发现C6H11Br分子解离过程中大部分能量都转化为内能, 但与其它长链溴代烷烃分子相比, 可资用能更多地被分配到平动能中, 结合软反冲模型分析了这种能量分配跟环烷基的构象和稳定性的关系.     

咔唑及其衍生物的质谱研究

本文报道咔唑和十三个N-取代咔唑衍生物(R=CH₃,C₂H₅,n-C₃H₇,n-C₄H₉,n-C₅H₁₁,n-C₆H₁₃,n-C₇H₁₅,CH₂CH₂Cl,CH₂CH₂Br,CH(CH₃)₂,CH=CH₂,CH₂CH=CH₂和CH₂C₆H₅)的质谱裂解过程。结果表明:1.这些化合物都显示分子离子峰,它们的相对丰度似有随R链的增长而减弱的趋势;2.当R为碳原子数大于1的直链烷基时,各化合物的质谱中都有相同的、以m/z180和m/z167为母离子的两个碎片离子系列,即m/z180;152,127,90和m/z167,166,140,139,115,113;3.当R为乙烯基时,重排断裂是主要途径;而R为烯丙基时,断裂方式与直链烷基衍生物的相同,但α-断裂是主要的;4.R为CH₂CH₂Cl和CH₂CH₂Br时,β-断裂也有一定几率;R为CH₂C₆H₅时,主要的断裂过程是产生m/z91的(艹卓)鎓离子。     

脂族酰基过氧化物分解动力学的研究(Ⅷ)——过氧化辛酰、过氧化己酰热分解产物的CIDNP效应

测定了过氧化辛酰(1)和过氧化己酰(2)在邻二氯苯中,分别在碘、碘乙烷、2-碘丙烷和3-溴丙烯存在下,90℃时热分解产物的¹HNMR谱,观察到自由基捕获产物(RX,R=n-C₇H₁₅、n-C₅H₁₁;X=I,Br)和歧化产物(R_-H)的CIDNP多重效应。讨论了过氧化酰热分解生成自由基对及相互作用的机理。     

自旋捕集EPR研究三种水合丁基钴肟光解Co-C键断裂产生的自由基的重排反应

以MNP为捕集剂,对三种水合丁基钴肟RCo(DH)₂H₂O(R=n-C₄H₉,#em/em#-C₄H₉,sec-C₄H₉)水溶液进行了光解EPR研究,发现其Co-C键断裂产生的自由基进一步重排的反应.     

2-溴噻吩和3-溴噻吩在267 nm的C-Br键解离机理

利用离子速度影像技术, 研究了2-溴噻吩和3-溴噻吩两种同分异构体在267 nm激光作用下的C—Br键解离机理, 获得了光解产物Br(2P3/2)和Br*(2P1/2)的能量和角度分布, 分析了两异构分子在267 nm 的C—Br键解离通道. 对于2-溴噻吩和3-溴噻吩, 产物Br来源于三个通道: (i) 从单重激发态系间窜跃到排斥的三重激发态的快速预解离; (ii)单重激发态内转化到高振动基态的热解离; (iii) 母体分子多光子电离后的解离. 2-溴噻吩的产物Br*具有类似的产生机制; 但对于3-溴噻吩, 从激发态内转换到高振动基态发生热解离成为产物Br*的主导通道, 而来自激发三重态的快速预解离通道则几乎消失. 定量地给出了各个通道的相对贡献、能量分配及各向异性分布信息. 实验发现, 随着溴原子在噻吩上取代位置远离硫原子, 来自通道(i)和(ii)产物之间的比例明显减小, 相应的各向异性分布有变弱趋势.     

2-溴噻吩和3-溴噻吩在267nm的C—Br键解离机理

利用离子速度影像技术,研究了2-溴噻吩和3-溴噻吩两种同分异构体在267 nm激光作用下的C-Br键解离机理,获得了光解产物Br(2P3/2)和Br*(2p1/2)的能量和角度分布,分析了两异构分子在267 nm的C-Br键解离通道.对于2-溴噻吩和3-溴噻吩,产物Br来源于三个通道:(i)从单重激发态系间窜跃到排斥的三重激发态的快速预解离;(ii)单重激发态内转化到高振动基态的热解离;(iii)母体分子多光子电离后的解离.2-溴噻吩的产物Br*具有类似的产生机制;但对于3-溴噻吩,从激发态内转换到高振动基态发生热解离成为产物Br*的主导通道,而来自激发三重态的快速预解离通道则几乎消失.定量地给出了各个通道的相对贡献、能量分配及各向异性分布信息.实验发现,随着溴原子在噻吩上取代位置远离硫原子,来自通道(i)和(ii)产物之间的比例明显减小,相应的各向异性分布有变弱趋势.     

微乳液体系相图的研究及其在纳米氟化物制备中的应用

绘制了十六烷基三甲基溴化铵(CTAB)/正丁醇(n-C₄H₉OH)/正辛烷(n-C₈H₁₈)/水[或NH₄F溶液、或Ba(NO₃)₂溶液、或KNO₃-Mg(NO₃)₂混合溶液]四组分微乳体系的拟三元相图.观察了电导率随水(或盐溶液)含量变化的规律,很好地印证了微乳液体系的相行为.选取相图中微乳区点作为最佳条件,制备了KMgF₃纳米粒子.     

溴代烷烃在紫外波段的光解离过程

在飞行时间质谱仪中，采用波长为234 nm和267 nm的激光，研究溴代烷烃CHBr3、CH2Br2、C2H5Br及C2H4Br2的光离解过程.在UV激光的作用下，溴代烷烃分子主要发生的是吸收1个光子解离出Br原子，然后继续吸收光子发生Br原子的（2＋1）共振增强多光子电离的过程.其中由溴代烷烃分子解离得到的Br原子可能存在着两种布居：基态Br(2P03/2)及激发态Br*(2P01/2).研究解离得到的Br原子的分支比 N(Br*)/N(Br)，并给出测量结果：溴代烷烃分子解离得到的Br原子在267 nm激光作用下的分支比明显大于在234 nm激光作用下的结果.对此多光子过程的机理，也进行了分析讨论.     

Velocity map imaging of the photolysis of n-C4H9Br in UV region

Using velocity map ion imaging technique, the photodissociation of n-C₄H₉Br in the wavelength range 231–267 nm was studied. The results and our ab initio calculations indicated that the absorption of n-C₄H₉Br in the investigated region originated from the excitations to the lowest three repulsive states, as assigned as 1A″, 2A′ and 3A′ in C_s symmetry. Dissociations occurred on the PES surfaces of the three states, terminating in C₄H₉+Br (²P_3/2) or C₄H₉ + Br^* (²P_1/2) as two channels, and being impacted by an avoided crossing between the PES surfaces of the 2A′ and 3A′ states. The transition dipole to the 1A″ state was perpendicular to the symmetry plane, so perpendicular to the C–Br bond. The transitions to the 3A′ state was polarized parallel to the symmetry plane, and also parallel to the C–Br bond. While the transition dipole to the 2A′ state was in the symmetry plane, but formed an angle of about 53.1° with the C–Br bond. We have also determined the avoided crossing probabilities, which affected the relative fractions of the individual pathways, for the photolysis of n-C₄H₉Br near 234 nm and 267 nm.     

The 1-bromoheptane photodissociation near 234 nm

The photodissociation of n-C₇H₁₅Br, near the red wing of the absorption A-band, has been investigated utilizing the velocity mapped ion imaging technique. Both the speed and angular distributions of Br^*(²P_1/2) and Br(²P_3/2) fragments were determined. The experimental data indicate that the photodissociation in the investigated range originates from adiabatic and non-adiabatic transitions of the three low-lying dissociative electronic states. The fragments kinetic energies and the angular distributions show that about 70% energy is deposited into the internal energy of the fragments. These results can be explained using soft impulsive model. The experiment also shows that the anisotropy parameter for Br^* is sensitive to the photolysis wavelength.     

Synthesis and properties of alkyldicyclopentadienyl-vanadium(III) compounds

The compounds Cp₂VR (R = CH₃, C₂H₅, n-C₃H₇, n-C₄H₉, n-C₅H₁₁, CH₂C(CH₃)₃ or CH₂Si(CH₃)₃) have been prepared from Cp₂ VCl and RMgX in n-pentane. The air-sensitive compounds are stable at room temperature, but decompose between 65 and 138°C. The thermal stability decreases in the order R = CH₃ CH₂Si(CH₃)₃ > C₂H₅ > CH₂C(CH₃)₃ > n-C₅H₁₁ > n-C₄H₉ > n-C₃H₇. Compounds with R = i-C₃H₇ or t-C₄H₉ could not be obtained.     

Synthese und reaktivität von dienylmetall-verbindungen : XXVII. Ein einfacher weg zur synthese von cyclopentadienylcobalt(III)-dikationen

CpCo(CO)₂ is oxidised by [Cp₂Fe]BF₄ (Cp = C₅H₅) in the presence of neutral ligands L to give the dications [CpCoL₃]²⁺ (L = SMe₂, S(n-C₄H₉)₂, PMe₃, C₅H₅N, MeCN; Me = CH₃). In [CpCo(SMe₂)₃]²⁺, sulfane ligands are substituted by neutral ligands L, L---L and L---L---L, to give the complexes [CpCoL₃]²⁺ (L = SeMe₂, TeMe₂, PMe₃, P(OMe)₃, AsMe₃, SbMe₃, t-C₄H₉NC, C₅H₅N, MeCN), [Cp-Co(L---L)SMe₂]²⁺ (L---L = R₂P(CH₂)_nPR₂, n = 1, 2, R = C₆H₅; bipyridine, o-phenanthroline, neocuproin) and [CpCo(L---L---L)]²⁺ (L---L---L = RP(CH₂CH₂PR₂)₂, R = C₆H₅). The dications react with iodide resulting in the monocations [CpCoL₂I]⁺ and [CpCo(L---L)I]⁺. Azacobaltocinium cations [CpCo(C₄R₂H₂N)]⁺ (R = H, CH₃) are obtained by reaction of [CpCo(SMe₂)₃]²⁺ with metal pyrrolides.     

双(烷基环戊二烯基)二硫氰基钛、锆、铪的合成

文献报道了双(环戊二烯基)二硫氰基钛、锆、铪^[1-3]及双(甲基环戊二烯基)二硫氰基钛^[4]的合成。我们利用双(烷基环戊二烯基)二氯化钛、锆、铪与过量硫氰酸钾反应,合成了一系列新的双(烷基环戊二烯基)二硫氰基钛、锆、铪(见表1)。     

Experimental Binary Phase Diagram of Bilayer Compounds [n-CnH2n+1N(CH3)3]2CoCl4

Compounds [n-C_nH_2n+1N(CH₃)₃]₂CoCl₄(n=16, C₁₆C₃Co; n=18, C₁₈C₃Co) containing lipid-like bilayers embedded in a crystalline matrix exist in solid-solid phase transition. The low-temperature bilayer structures of the two compounds were organized by neutralizing CoCl₄^2- with alkylammonium ions. Alkyl chains lay parallel to each other and slightly tilted with respect to the normal of the inorganic layers. The adjacent alkyl chains interacted with each other by van der Waals interaction. When the temperature increased, the two compounds underwent a reversible solid-solid phase transformation within 310―330 K. In such a case, the chains showed a large motional freedom, and a disordered phase appeared. The structures can alternatively be viewed as a double layer of alkylammonium ions between CoCl₄^2- sheets and be considered as crystalline models of lipid bilayers. The experimental subsolidus binary phase diagram of [n-C₁₆H₃₃N(CH₃)₃]₂CoCl₄-[n-C₁₈H₃₇N(CH₃)₃]₂CoCl₄ was constructed over the entire composition range by differential scanning calorimetry and X-ray diffraction technique. Experimental phase diagram indicates one stable intermediate phase [n-C₁₆H₃₃N(CH₃)₃][n-C₁₈H₃₇N(CH₃)₃]CoCl₄ at w_C16C3Co= 39.89% and two invariant three- phase equilibria, which shows two eutectoid temperatures: T_e1 at (316±1) K for w_C16C3Co= 27.35% and T_e2 at (313±1) K for w_C16C3Co=59.76%. These three noticeable solid-solution ranges are α-phase at the left, β-phase at the right, and γ-phase in the middle of the phase diagram.     

硼化合物研究(Ⅲ)——B10H102-、B12H122-以及B3H8-阴离子的二茂铁季铵盐的合成

本文通过B_nH_n^2-(n=10,12)及B₃H₈^-盐分别与C₅H₅FeC₅H₄CH₂N(R)Me₂Cl和Fe(C₅H₄CH₂N(R)Me₂Cl)₂(R=CH₃-,C₂H₅-,n-C₃H₇-,CH₂=CH-CH₂-和CH≡C-CH₂-)在水溶液中进行反应,合成了相应的三十个新的硼烷阴离子衍生物,这些化合物对水稳定性好,B₁₀H₁₀^2-及B₁₂H₁₂^2-衍生物对热、酸、碱和氧化剂均很稳定。研究了反应物之间的用量比例对反应产物的影响。实验结果表明,不论反应物之间的克分子比如何变化,只能得到相应的一种产物(产率90-98％)。     

The decomposition of C4H8 complexes at controlled internal energies

A coincidence technique is used to study the influence of the internal energy of the reactant ion on the cross section of the ion-molecule reactions in the C₂H₄⁺ + C₂H₄ system. The experiment is performed at thermal collision energies. In the ion-molecule reactions of C₂H₄⁺ + C₂H₄ our measurements indicate a barrier between the initially formed collision complex (C₂H₄)₂⁺* and a tight complex (C₄H₈⁺)*. Using an extension of our earlier developed statistical model, now including a potential barrier between the initially formed loose complex (C₂H₄)₂⁺* and the tight complex (C₄H₈⁺)*, our experimental data can be reproduced. For comparison also the internal energy dependence of the unimolecular decomposition of photoionised 1-C₄H₈⁺ is measured. Assuming that the photoionised 1-C₄H₈⁺ is identical with the tight (C₄H₈⁺)* complex, the model applied to the ion-molecule reactions describes also the unimolecular decay of 1-C₄H₈⁺ correctly, using the same set of parameters.     

Interaction of heterocyclic thioamides with tellurium(II) and tellurium(IV). Syntheses and crystal structures of bis[2-(2-thioxo-1,3- thiazolidin-3-yl)-4,5-dihydro-1,3- thiazolium]hexabromotellurate(IV) and tris(1- methylimidazole-2-(3H)-thione)tellurium(II) bromide

Reaction of 1,3-thiazolidine-2-thione with tellurium(IV) in hydrobromic acid medium gave the hexabromotellurate, [C₆H₉N₂S₃]₂²⁺[Te^IVBr₆]²⁻ (3). Reaction of 1-methylimidazoline-2-(3H)-thione (L″) with tellurium(IV), in hydrobromic acid medium, gave the mixed-ligand tellurium(II) complex [Te^IIL″₃Br]⁺Br⁻ (4). The structures of [C₆H₉N₂S₃]₂²⁺[Te^IVBr₆]²⁻ (3) and [Te^IIL″₃Br]⁺Br⁻ were determined by single crystal X-ray diffraction methods. In 3 the unit cell contains [TeBr₆]²⁻ anions and two [C₆H₉N₂S₃]⁺ cations. There is no direct bonding between the metal atom and the cations. In the anion only slight angular deviations from the perfect octahedral geometry are observed. The lone pair of electrons on tellurium(IV) is found to be stereochemically inert. In the cation the two five-membered heterocyclic rings adopt different conformations. In complex 4, in the solid state, the planar [Te^IIL″₃Br]⁺ cation and Br⁻ anion are held together by ionic interactions. In the cation, L″ is bonded to the central tellurium atom through the sulphur atom.